Potential of an undefinided cylinder

AI Thread Summary
The discussion revolves around calculating the electric potential created by an infinitely long, uniformly charged cylinder with radius R and density ρ. Participants emphasize the use of Gauss's law to derive the electric field both inside and outside the cylinder. The electric field inside is given as E = ρr / (2ε₀), while outside it is E = ρR² / (2ε₀r). The connection between electric field and electric potential is highlighted, indicating that integration is necessary to find the potential, particularly for points outside the cylinder, which remains a challenge for one participant. The conversation underscores the importance of clear mathematical representation and understanding the concepts of electric fields and potentials in electrostatics.
Guillem_dlc
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Homework Statement


Determine the potential that creates an undefined cylinder of radius $R$ and density density $\rho$ that is uniformly charged.

Homework Equations


Gauss's law.

The Attempt at a Solution


I know that for this problem I can use gauss because it is a cylinder, now I do not get anywhere right, it is also a question of calculating the potential. Some help? Besides, the indefinite thing confuses me a little ...
 
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I venture to guess that the problem statement is to be interpreted as asking for the potential created by an infinitely long cylinder of radius ##R## and uniform volume charge density ##\rho##.

Please show the details of your attempt of using Gauss' law.
 
TSny said:
I venture to guess that the problem statement is to be interpreted as asking for the potential created by an infinitely long cylinder of radius ##R## and uniform volume charge density ##\rho##.

Please show the details of your attempt of using Gauss' law.
Yes, of course I'll pass it to you. I think that's fine by now.
 

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It's preferable to type out your equations rather than post pictures. That way, we can easily quote specific parts of your calculations.

In your final expression for ##\vec E##, I take it that the symbol circled in green
upload_2018-3-19_16-49-23.png
should be ##r##. If so, then it looks OK. But is this the electric field at a point inside the cylinder or at a point outside the cylinder?
 

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TSny said:
It's preferable to type out your equations rather than post pictures. That way, we can easily quote specific parts of your calculations.

In your final expression for ##\vec E##, I take it that the symbol circled in green View attachment 222331 should be ##r##. If so, then it looks OK. But is this the electric field at a point inside the cylinder or at a point outside the cylinder?
Yes it is a [ tex ] r [ / tex ] sorry it is not clear. It's the field for the interior I think.
 
Guillem_dlc said:
It's the field for the interior I think.
OK, that's correct. Are you trying to get the potential at a point inside the cylinder, outside the cylinder, or both?

What is the connection between electric field and electric potential?
 
TSny said:
OK, that's correct. Are you trying to get the potential at a point inside the cylinder, outside the cylinder, or both?

What is the connection between electric field and electric potential?
We have seen that ##\vec{E}=\rho \dfrac{r}{2\varepsilon_0}\vec{r}## is in the inside of the cylinder.
Also, ##E2\pi rh=\dfrac{1}{\varepsilon_0}\rho V\Rightarrow E=\dfrac{\rho \pi R^2h}{2\pi rh\varepsilon_0}\Rightarrow \vec{E}=\dfrac{\rho R^2}{2\varepsilon_0r}\vec{r}## is outside the cylinder.
The connection between electric field and electric potential: one is the derivative of the other, is not it? Would I have to integrate in this case? But I do not know anymore.
 
  • #10
Please show your work.
 
  • #11
TSny said:
Please show your work.
I have solved the ##V (r)## for ##r <R## (inner points).
##V(r)=\int_r^0 \vec{E}\cdot d\vec{l}=\int_r^0\dfrac{\rho r}{2\varepsilon_0}\vec{a}_r\cdot d\vec{l}=\dfrac{\rho}{2\varepsilon_0}\int_r^0rdr=\dfrac{\rho}{2\varepsilon_0}\left[ \dfrac{r^2}{2}\right] _r^0=-\dfrac{\rho r^2}{4\varepsilon_0}##
 
  • #12
Guillem_dlc said:
I have solved the ##V (r)## for ##r <R## (inner points).
##V(r)=\int_r^0 \vec{E}\cdot d\vec{l}=\int_r^0\dfrac{\rho r}{2\varepsilon_0}\vec{a}_r\cdot d\vec{l}=\dfrac{\rho}{2\varepsilon_0}\int_r^0rdr=\dfrac{\rho}{2\varepsilon_0}\left[ \dfrac{r^2}{2}\right] _r^0=-\dfrac{\rho r^2}{4\varepsilon_0}##
This looks right. Note that you are taking the potential to be zero at ##r = 0##, which is a good choice for this problem.
 
  • #13
Have you also been able to get the potential at points outside the cylinder?
 
  • #14
No
 
  • #15
Guillem_dlc said:
No
What is it about points outside the cylinder that is making it difficult to find the field and potential?
 
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